The triplet basis functions for the odd pairing channels are shown in Table REF . In the \(\Gamma _7\)  and \(\Gamma _8\)  bands we have \(\hat{\cal R}(g)=\hat{R}\)  for all \(g\) , therefore \( {d} \)  and \( {e} _\mu \) 
transform under rotations like vectors and the standard expressions for the basis functions[1]}, [2]} are applicable. In contrast, in the \(\Gamma _9\)  bands we have \(\hat{\cal R}(g)\ne \hat{R}\)  for some \(g\) ,
therefore \( {d} \)  and \( {e} _\mu \)  do not transform under all rotations like vectors, which changes the momentum dependence of the basis functions.[3]} Note that all three components of \( {d} \)  never
vanish simultaneously in a whole plane in the momentum space, so that Blount's theorem about the absence of line nodes in a generic triplet state[4]} holds in the exceptional non-pseudospin bands as well.
